POLYMER-DISPERSED FERROELECTRIC LIQUID CRYSTAL DISPLAY

Abstract: The present invention discloses a novel Polymer-Dispersed Ferroelectric Liquid Crystal Display (PDF LCD). The active matrix LCD such as a TFT LCD, the solution of low response speed of nematic LCD, requires very high production costs. And the FLCD utilizing ferroelectric liquid crystal exhibits highly rapid response speed, but results in an unstable structure, difficult fabrication, and incompetency of expressing gray scales. Meanwhile, the PD LCD exhibits a simple structure, wide viewing angle and high strength, but low contrast thereof disqualifies it for the image display. The present invention combines the PD LCD and FLCD that is dispersing droplets of ferroelectric liquid crystal in a polymer matrix to compensate merits and dismerits of them. As the result, there is provided a novel PDF LCD having very rapid response speed, toughness to external shock or heat, and high contrast. Moreover, the present PDF LCD does not exhibit bistable characteristics to be able to express gray scales, and thus it is suitable for fabricating large area color image display.

Description: POLYMER-DISPERSED FERROELECTRIC LIQUID CRYSTAL DISPLAY TECHNICAL FIELD The present invention relates to a liquid crystal display(LCD), and particularly to a novel LCD fabricated by dispersing ferroelectric liquid crystal(FLC) in a polymer matrix. BACKGROUND ART A Braun tube is generally adopted as the display for an image displaying apparatus such as a television. The Braun tube, however, has excessively large dimensions, and exhibits very high power consumption. Thus, the flat panel display(FDP) recently comes into wide use especially for the field of portable displays. Among these FDPs, the LCD is most widely being used. The LCD is a typical non-emissive display utilizing electro-optic characteristics of liquid crystal(LC), for example the dielectric anistropy. Liquid crystal is divided into smectic, nematic and cholesteric phases according to their molecular structures. Among them, smectic and nematic LC can be used for the purpose of display, but the smectic LC is not easily be aligned and the alignment is not stable under heat or shock, most of practical LCDs, therefore, adopt nematic LCs. As the nematic LCD, TN(Twisted Nematic) or STN(Super Twisted Nematic) LCDs have been used. TN or STN LCDs are constructed by aligning LC molecules to relatively twisted directions at upper and lower surfaces of the LC layer, and are already been widely used. But, they can not fulfill the rapid response speed and the viewability, such as an wide viewing angle, necessary for achieving the high resolution and the large screen. Accordingly, full-color or dynamic images can not easily be achieved by these nematic LCDs. Moreover, they cannot be easily driven, as the optical response of simple matrix type nematic LCDs, depens upon the square of the applied voltage to result in little level difference between the selected and non- selected pixels. As the result, the nematic LCD can only be applied up to the portable television or the monitor of the notebook computer with unsatisfactory image quality. Then, a TFT(Thin Film Transistor) LCD of an active matrix type is developed, it enables a high speed action by independently switching each of pixels by an array of driving elements. But it has a highly complicated structure to require high production cost and bring about difficulty in fabricating a large screen. All of above described LCDs require the alignment of LC molecules to prescribed directions at boundary surfaces of LC, and use separate polalizers, to narrow the viewing angle and deteriorate the brightness. Thus, a Polymer-Dispersed (PD) LCD is developed. It adopts the structure of dispersing submicron- sized mematic LC droplets in a polymer matrix. As the nematic LC has the positive dielectric anistropy responding to the external electric field, it maintains the opaque state by scattering incident lights when the electric field is not applied. When the electric field is applied, LC molecules of LC droplets are aligned to one direction to be a transparent state, and allow to pass the light. As the PD LCD does not adopt the polarizer to result is a simple structure, a high brightness, and an wide viewing angle. Moreover, its polymer structure enables a flexible large LCD of a high strength at a low porduction cost. In the PD LCD, however, the driving voltage is applied to LC through the polymer matrix, thereby revealing a high operating voltage, a large power consumtion, and a low contrast. As the result, it can be utilized to control the lighting of the window, and not suitable for the image display such as a television. All of above described LCDs utilizes the dielectric anistropy of LC, and the electro -optic characteristics thereof depends upon only the strength of applied voltage, regardless of its polarity. On the contrary, ferroelectric material is spontaneously polarized even if the electric field is not applied to exhibits so-called bistable structure with two stable states. Recently, there has been reported that a smectic LC of chiral -C phase exhibits the ferroelectricty with a very high spontaneous polarization, and it is adopted to a Ferroelectric LCD(FLCD). In the FLCD, the direction of LC molecules is changed between two states without any alteration of the molecular structure, thus reveals a highly rapid response speed regardless of the viscosity of LC. While the nematic LCD has the response speed of tens or hundreds of milli seconds (ms), the FLCD reveals much faster response speed of tens of micro seconds (us). Therefore, the FLCD overcomes the limit of the information content of the STN LCD, and reduces the production cost and initial investment comparing with the TFT LCD. But, the chiral-C phased smectic LC is not easily be aligned, and the alignment structure is easily changed by external shock or heat, thus results in low reliability. Moreover, the thickness of LC layer, namely the gap between two substrates should be reduced to prevent the spiral movement of LC due to the chiral characteristic, and to align LC to prescribed directions. Thus, The conventional FLCD forms the gap between sabstrates at 1 to 2 μm, and is referred to as Surface Stabilized (SS) FLCD. But it is very difficult to uniformly keep this small gap all over the large area, thus the fabrication of large FLCD, especially SS FLCD, is practically impossible. While the other voltage dependent LCDs can express gray scales by controlling the strength of the electric field, the FLCD is impossible to represent intrinsic gray scales, as the FLCD has only two states of aligned directions of LC molecules according to the polarity of the external electric field. DISCLOSURE OF THE INVENTION In consideration of drawbacks of above described various conventional LCDs, an object of the present invention is to provide a novel Polymer-Dispersed Ferroelectric Liquid Crystal Display(PDF LCD) for taking merits and compensating dismerits of the PD LCD and the FLCD. To achieve the above object, the PDF LCD according to the present invention, having two substrates opposing at a prescribed gap, two grids respectively arranged on the substrates and being opposed each other, and an LC layer filled in a cavity between two substrates, characterized in that: the LC layer being constructed by dispersing ferroelectric LC droplets in a polymer matrix. According to one aspect of the present invention, the ferroelectric LC is smectic LC of chiral-C phase. According to another aspect of the present invention, the LC filled between substrates is aligned to prescribed directions at each of its boundary surfaces, and is preferably aligned by rubbing an alignment layer. According to other aspect of the present invention, means for polarizing, such as polarizers, is provided on substrates. The resultant PDF LCD according to the present invention reveals an wide viewing angle and a high strength as those of a PD LCD, and the rapid response speed as that of an FLCD. And it overcomes the drawback of PD LCD to provide a high contrast image, and resolve the alignment and gray scale problems of the FLCD, to provide a reliable alignment structure of stable characteristics, and make it possible to express intrinsic gray scales. And the cell gap of the PD FLCD should not be formed in a small gap, as of the SS FLCD, thus the fabrication of the PD FLCD becomes easy and thus a large LCD can easily be constructed. BRIEF DESCRIPTION OF DRAWINGS These and other objects and advantages of the present invention will be more apparent form the following detailed description, with reference to the accompanying drawings, in which: FIG. 1 is a schematic sectional view depicting the PDF LCD according to the present invention; FIG. 2 is a graph showing the response of the PDF LCD to a square wave; FIG. 3 is a graph illustrating the change of electro-optic characteristics of the PDF LCD according to the change of applied voltage; and FIG. 4 is a graph showing the response speed of the PDF LCD according to the present invention. Referring to FIG. 1, a PDF LCD according to the present invention comprises an LC layer L formed by dispersing LC droplets D in a polymer matrix M, in a cavity, or cell gap, between front and rear substrates F, R. This structure is basically similar to that of PD LCD. The LC to form the LC droplets, however, is ferroelectric LC exhibiting the spontaneous polarization, in the present invention. The ferroelectric LC is smectic LC of chiral-C phase, for example. And the present LCD requires an alignment structure to utilize electro-optic characteristics of ferroelectric LC, comparing with the PD LCD using the scattering mode. On inner surfaces of two substrates F, R, grids Gl, G2 are arranged in the form of a matrix, for applying voltage to select pixely, and they are preferably consisted of transparent conductive material, such as ITOdndium Tin Oxide). Meanwhile, alignment layers A are respectively formed on grids Gl, G2 to align LC molecules in the droplet D to prescribed directions. The layer A is used not only for aligning LC, but also for preventing direct inflow of current from grids Gl, G2 to LC. And the layer A can be formed of pol imide, which is generally used for aligning TN or STN LCD, and other polymer or aligning means other than the alignment layer A can be adopted if necessary. The polyimide layer can stably align LC molecules in LC droplets D to a prescribed direction, after being rubbed to certain directions. At outer surfaces of each substrates F, R, polarizers PI, P2 are respectively attached for linearly polarizing the incident light to one direction, thereby allowing or blocking the pass of the light. Thus, the optical black and white states are formed to express the information. And remaining numeral S desinates the sealing wall. Though it is not depicted plainly, spacers of glass or synthetic resin are uniformly dispersed in the cell gap between two substrates F, R to maintain the gap between two substrates F, R even. Now, procedures to fabricate a sample of the above described PDF LCD accordig to the present invention, will be described. Firstly, a test panel having a cell gap for being filled with LC layer L, is prepared. The test panel is fabricated by coupling two substrates F, R with the sealing wall S, and each of substrates F, R respectively has grids Gl, G2 and alignment layers A aligned to prescribed directions. In this example, the thickness of the cell gap, namely the thickness of the LC layer L is selected to be 9.6um. Then, LC and polymer to form the LC layer L is mixed at a prescribed mixing ratio. If the amount of LC is excessive, LC droplets D and polymer matrix M can not be completely separated in the phase separation, while the electro-optic characteristics is deteriorated in the defficient case. Accordingly, the selection of an appropriate mixing ratio is very important. In the example, CS 2004 (trade name) of Chisso is adopted as chiral-C phased smectic LC, and NOA61 UV(Ultra Violet) curable polymer is adopted as polymer. According to the present inventor's tests, the range of 1: 1.5 to 1:10 in weight seems to be appropriate for the mixing ratio of LC and polymer, and LC and polymer are mixed in the weight ratio of 1:3 in the example. After that, the mixture of LC and polymer is injected to the cell gap of the test panel. The temperature at the point of the injection, is preferable to be relatively high for preventing the separation of the mixture and resultant stain, due to the viscosity difference between LC and polymer. The temperature at the point of the injection is preferable to be around the phase transition temperature at which LC is changed from the LC phase to the isotropic liquid phase, and the temperature is selected to be 120 in the example. If the UV is applied immediately after the injection of the mixture, the mixture is cured before the flow is stabilized, thus the mixture is kept still for a prescribed time at the above described temperature. In the example, the mixture is kept under the phase transition temperature of LC, for example 120 "C, for ten minutes. According to the present inventor's tests, LC and polymer will not be uniformly mixed but separated, if the keeping temperature is low, while the effect of the alignment is reduced if high. Thus, the selected keeping temperature corresponds to the temperature as low as two materials may be uniformly mixed. Then, LC and polymer is phase separated by radiating UV. In the phase separation, higher ambient temperature or higher radiation intensity of UV accelerates the curing speed to reduce the size of the LC droplet D. Therfore, the size of the LC droplet D can be adjusted by controlling ambient conditions as described above. According to the present inventors tests, appropriate optical characteristics are obtained when the diameter of the LC droplet D is in the range of 0.5um to lOum. In that case, the gap between two substrates F, R, namely the thickness of the LC layer L or the cell gap, will be preferable to be the value at which LC droplets D can be enoughly dispersed in the cured polymer matrix M, for example in the range of 2Um to lOum. Meanwhile, two polarizers PI, P2 are respectively attached to outer surface of substrates F, R, and attached angles thereof will be determined by the angle at which an optimum contast can be obtained according as the tilt angle of LC. In the example, one polarizer PI is attached at the angle of 22.5° , and the other polarizer P2 perpendicular with each other. Electro-optic characteristics of the example of the PDF LCD fabricated as described above, will now be described with reference to FIG. 2 to FIG. 4. Referring to FIG. 2, there is shown the electro-optic response of the present LCD, when the pulse of square wave formed voltage of 500Hz is applied to the example. As shwon in the drawing, the PDF LCD according to the present invention, responds very well to the change of the external electric filed, thus can be used for electro-optic display element. Now referring to FIG. 3, the intensity of light after passing two polarizers PI, P2 when the voltage of the squre wave is varied. As shown in the drawing, the PDF LCD according to the present invention responds linearly at the low voltage, and is smoothly saturated as the voltage goes high. In other words, the PDF LCD according to the present invention does not reveal the bistable characteristics as of the SS FLCD, but exhibits a continuous light passing characteristics according to the change of the external applied voltage. Therefore, the expression of intrinsic gray scales can be achieved by changing the applied voltage. Referring to FIG. 4, there is shown the response speed of the present LCD according as the change of the external electric field. As shown in the drawing, the PDF LCD according to the present invention exhibits the response speed of about 0.1ms, i.e. lOOus. The PDF LCD is relatively not faster than the FLCD which exhibits the response speed of tens of Us, but is much faster than the nematic LCD revealing tens of ms. As described above, the present invention combines the PD LCD and FLCD to compensate merits and dismerits of them. But the present PDF LCD reveals novel electro-optic characteristics which cannot be anticipated from a simple combination of the PD LCD and the FLCD. Thus, the PDF LCD according to the present invention, exhibits a rapid response and high contrast as in the conventional FLCD, and remedies drawbacks of the FLCD to get a stable alignment and to express gray scales. And the thickness of the cell gap may not be formed in small as in the SS FLCD, thus a large LCD can be easily fabricated. Moreover, the PDF LCD according to the present invention has an excellent strength as in PD LCD, thus a strong LCD tough to the external shock or impact can be fabricated. And its wide viewing angle also exhibits an excellent viewability. Especially, the present PDF LCD exhibits the rapid response speed without any active matrix drive as in the TFT LCD, thus excludes the necessity of any active elements to drastically reduce production costs. INDUSTRIAL APPLICABILITY These various characteristics of the present PDF LCD will be suitable for displaying color images on a large screen, thus the present invention facilitates the fabrication of large area color display, such as a high definition television.

Claims: CLAIMS 1. In a liquid crystal display having two substrates F, R opposing at a prescribed gap, two grids Gl, G2 respectively arranged on said two substrates F, R and being opposed each other, and a liquid crystal layer L filled in a cavity between said two substrates F, R, a polymer- dispersed ferroelectric liquid crystal display (PDF LCD) characterized in that: said liquid crystal layer L being constructed by dispersing droplets D of ferroelectric liquid crystal in a polymer matrix M. 2. A PDF LCD according to claim 1, wherein said ferroelectric liquid crystal is smectic liquid crystal of chiral-C phase. 3. A PDF LCD according to claim 1, wherein said liquid crystal is aligned to prescribed directions respectively at two boundary surfaces of said liquid crystal layer L. 4. A PDF LCD according to claim 3, wherein said alignment is accomplished by coating polymer material on said grids Gl, G2; and rubbing said polymer coating. 5. A PDF LCD according to claim 4, wherein said polymer material to be rubbed is polyimide. 6. A PDF LCD according to claim 1, wherein means for polarizing is further comprised on said substrates F, R. 7. A PDF LCD according to claim 6, wherein said polarizing means is polarizers PI, P2 which linearly polarize incident light. 8. A PDF LCD according to claim 1, wherein the diameter of said droplets D in said polymer matrix M is in the range of 0.5|im to lOum. 9. A PDF LCD according to claim 1, wherein the thickness of said liquid crystal layer L is in the range of 2um to lOum. 10. A PDF LCD according to claim 1, wherein said liquid crystal layer L is constructed by injecting the mixture of said ferroelectric liquid crystal and said polymer to said cavity between said two substrates F, R; and phase separating and curing said mixture. 11. A PDF LCD according to claim 10, wherein the mixing ratio of said ferroelectric liquid crystal and said polymer is in the range of 1:1.15 to 1: 10 in weight. 12. A PDF LCD according to claim 10, wherein the temperature at the state of injecting said mixture, is about the phase transition temperature of said liquid crystal. 13. A PDF LCD according to claim 10, wherein said mixture is kept for a prescribed time at a prescribed temperature after said injection; and then, phase separated and cured. 14. A PDF LCD according to claim 10, said polymer is UV curable; and said phase separation and curing of said mixture is accomplished by the radiation of UV.

Inventors: LEE KYE HUN, LEE SIN DOO, SUH SEONG WOO, LEE, KYE, HUN, LEE, SIN, DOO, SUH, SEONG, WOO
Applicants: LEE KYE HUN, LEE SIN DOO, ORION ELECTRIC CO LTD, SUH SEONG WOO, LEE, KYE, HUN, LEE, SIN, DOO, ORION ELECTRIC CO., LTD., SUH, SEONG, WOO
Application year: 1994
Main classification: G02F1
IPC codes: G02F1